Cargando…

Influence of wide band gap oxide substrates on the photoelectrochemical properties and structural disorder of CdS nanoparticles grown by the successive ionic layer adsorption and reaction (SILAR) method

The photoelectrochemical properties of nanoheterostructures based on the wide band gap oxide substrates (ZnO, TiO(2), In(2)O(3)) and CdS nanoparticles deposited by the successive ionic layer adsorption and reaction (SILAR) method have been studied as a function of the CdS deposition cycle number (N)...

Descripción completa

Detalles Bibliográficos
Autores principales: Malashchonak, Mikalai V, Mazanik, Alexander V, Korolik, Olga V, Streltsov, Еugene А, Kulak, Anatoly I
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Beilstein-Institut 2015
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4685871/
https://www.ncbi.nlm.nih.gov/pubmed/26734517
http://dx.doi.org/10.3762/bjnano.6.231
Descripción
Sumario:The photoelectrochemical properties of nanoheterostructures based on the wide band gap oxide substrates (ZnO, TiO(2), In(2)O(3)) and CdS nanoparticles deposited by the successive ionic layer adsorption and reaction (SILAR) method have been studied as a function of the CdS deposition cycle number (N). The incident photon-to-current conversion efficiency (IPCE) passes through a maximum with the increase of N, which is ascribed to the competition between the increase in optical absorption and photocarrier recombination. The maximal IPCE values for the In(2)O(3)/CdS and ZnO/CdS heterostructures are attained at N ≈ 20, whereas for TiO(2)/CdS, the appropriate N value is an order of magnitude higher. The photocurrent and Raman spectroscopy studies of CdS nanoparticles revealed the occurrence of the quantum confinement effect, demonstrating the most rapid weakening with the increase of N in ZnO/CdS heterostructures. The structural disorder of CdS nanoparticles was characterized by the Urbach energy (E(U)), spectral width of the CdS longitudinal optical (LO) phonon band and the relative intensity of the surface optical (SO) phonon band in the Raman spectra. Maximal values of E(U) (100–120 meV) correspond to СdS nanoparticles on a In(2)O(3) surface, correlating with the fact that the CdS LO band spectral width and intensity ratio for the CdS SO and LO bands are maximal for In(2)O(3)/CdS films. A notable variation in the degree of disorder of CdS nanoparticles is observed only in the initial stages of CdS growth (several tens of deposition cycles), indicating the preservation of the nanocrystalline state of CdS over a wide range of SILAR cycles.